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Theoretical study of electron dynamics in graphene interacting with ultrafast and ultrastrong laser pulses

机译:石墨烯电子动力学与超空气和超空脉冲脉冲的理论研究

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In this paper, we investigate the dynamics of electron system in graphene monolayer from the theoretical and numerical points of view. We have shown that graphene subjected to an ultrafast (near-single-oscillation pulse) and strong (on the order of interatomic field) pulse, exhibits fundamental behavior dramatically different from both insulators and metals. In such an ultrafast and ultrastrong field, the electron dynamics is coherent and is described by time-dependent Schrodinger equation. Electron transfer from Valence band to Conduction band is deeply irreversible which implies non-adiabaticity of the system in which the residual Conduction band population (after the pulse ends) is close to the maximum one. The residual Conduction band populations a function of wave vector is non-uniform with a few strongly localized spots near the Dirac points, at which the Conduction band is almost fully populated.
机译:在本文中,我们从理论和数值视角调查石墨烯单层中电子系统的动态。我们已经表明,经过超快(近单振荡脉冲)和强(在内部田间)脉冲的强(在近单振荡脉冲)脉冲的石墨烯,从绝缘体和金属呈现出显着不同的基本行为。在这种超快和超空地中,电子动力学是相干的并且由时间依赖的Schrodinger方程描述。从价带向导带的电子转移深入不可逆,这意味着剩余传导频带群体(脉冲端后)接近最大的系统的非绝热性。残留的传导频带群体的波向量的功能是不均匀的,并且在狄拉科附近的少量局部斑点,传导频带几乎完全填充。

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